Plasma processing method and method for manufacturing an electronic device
Summary by NHIP
Plasma Oxynitriding Method
The method generates plasma using nitrous oxide gas introduced below an upper shower plate. Electron temperature remains below 2.24 eV while gas enters through square openings in a lower shower plate supplied by a single gas discharge tube.
Claim Score by NHIP
Abstract
The application of oxynitriding treatment to electronic appliances involve the problem that N2 ions are formed to thereby damage any oxynitride film. It is intended to provide a method of plasma treatment capable of realizing high-quality oxynitriding and to provide a process for producing an electronic appliance in which use is made of the method of plasma treatment. There is provided a method of plasma treatment, comprising generating plasma with a gas for plasma excitation and introducing a treating gas in the plasma to thereby treat a treatment subject, wherein the treating gas contains nitrous oxide gas, this nitrous oxide gas introduced in a plasma of <2.24 eV electron temperature, so that the generation of ions tending to damage any insulating film is reduced to thereby realize high-quality oxynitriding. Further, there is provided a process for producing an electronic appliance in which use is made of the method of plasma treatment.

Term
Projected expiry 27 September 2026.
- Priority and filed
- Granted
- Today
- Projected expiry
4 claims: 1 independent, 3 dependent
- 1Broadest claimClaim Score 52, average(NHIP)A plasma processing method in which plasma is generated by the use of a plasma excitation gas and process gas is introduced into said plasma to thereby process an object to be processed, the method comprising:introducing said plasma excitation gas into a process chamber from an upper shower plate;generating said plasma under said upper shower plate;causing said plasma to pass through a lower shower plate provided under said upper shower plate so as to reach said object to be processed;and introducing said nitrous oxide gas, as said process gas, from said lower shower plate into the plasma whose electron temperature is less than binding energy 2.24 eV between a nitrogen molecule and an oxygen atom in said nitrous oxide, said nitrous oxide gas being introduced into the plasma under said lower shower plate, wherein said nitrous oxide gas is provided to said lower shower plate from a gas discharge tube provided at only one end of said lower shower plate, to thereby be discharged through respective openings of said lower shower plate into the process chamber.
89 paragraphs in 8 sections, as filed
TECHNICAL FIELD
0001This invention relates to a plasma processing method in which an object to be processed, such as a semiconductor substrate, and a substrate for a liquid crystal display or the like, is subjected to processing such as oxidation, nitridation, oxynitridation or the like and to a manufacturing method for manufacturing an electronic device such as a semiconductor device by the use of such a plasma processing method.
BACKGROUND ART
0002As a conventional plasma processing apparatus, use has been made of an apparatus as described in Patent Document 1. As described in Patent Document 1, this plasma processing apparatus comprises a radial line slot antenna adapted to radiate a microwave into a process chamber, a phase delay plate adapted to compress the wavelength of the microwave radiated from the antenna, a cover plate disposed at an interval from the phase delay plate, and a dielectric member disposed immediately below the cover plate. Further, a construction having a number of gas outlets is disposed under the dielectric member at an interval therefrom.
0003A gas for plasma generation is supplied into a vacuum container. When the microwave is applied from the antenna in this state, a high-density plasma is generated in a space between the dielectric member and the construction. This plasma is introduced through the construction into a process space where a semiconductor wafer is processed. With such a configuration, a process gas ejected from the gas outlets of the construction is excited by the high-density plasma formed under the dielectric member.
0004In this case, a flange constituting the process container is formed with a plasma gas supply passage communicating with a plasma gas inlet provided in an outer wall of the process chamber. From the plasma gas inlet, the plasma excitation gas such as Ar or Kr is fed to the supply passage in the flange. Further, the excitation gas is introduced into the process chamber through the supply passage and a gas outlet of the flange.
0005In the foregoing plasma processing apparatus having the radial line slot antenna, the uniform high-density plasma is formed in the space immediately below the dielectric member.
0006Patent Document 1:
0007Japanese Unexamined Patent Application Publication (JP-A) No. 2001-500327
DISCLOSURE OF THE INVENTION
Problem to be Solved by the Invention
0008Conventionally, an oxynitriding process of a substrate is carried out at a high temperature of 600° C. to 800° C. and there is known a problem that dopants are rediffused due to this high temperature process.
0009Therefore, as known from Japanese Unexamined Patent Application Publication No. 2000-294550, there is cited a plasma oxynitriding process that accelerates oxynitriding by a plasma at low temperature so as to prevent the rediffusion. However, there is known a problem that, simultaneously, an object to be processed is damaged due to the plasma process.
0010According to experiments by the present inventors, a problem has been found that leakage current increases on the low electric field side by introduction of an oxynitriding process gas into the inside in a plasma oxynitriding process.
0011An object of this invention is to provide a technique for clearing up the cause of various faults inherent to the foregoing oxynitriding process and enabling to reduce those faults.
0012A specific object of this invention is to provide a plasma process that can realize high-quality oxynitriding.
0013As a result of examining the cause of the foregoing faults, the present inventors have found a problem that excessive dissociation is accelerated by introduction of nitrous oxide into the inside of a plasma so that N<sub>2 </sub>ions are produced to damage a formed oxynitride film.
0014In view of this, this invention proposes a manufacturing method using a plasma processing apparatus capable of reducing the production of ions that damage an insulating film and of uniformly and efficiently supplying oxynitriding species in the plane of a process substrate.
Means for Solving the Problem
0015According to one mode of this invention, when nitrous oxide is used as an oxynitriding process gas, the electron temperature in a plasma is approximately 3.0 eV in a conventional plasma process. On the other hand, the binding energy between a nitrogen molecule and an oxygen atom is approximately 2.24 eV in nitrous oxide.
0016Therefore, if nitrous oxide is introduced into a plasma whose electron temperature is equal to or less than this nitrous oxide binding energy, it is possible to reduce the excessive dissociation.
0017Further, even in the case of another oxynitriding process gas such as ammonia, not limited to nitrous oxide, it is possible to reduce the production of N<sub>2 </sub>ions by suppressing excessive dissociation, thereby improving the properties of an oxynitride film.
0018According to an aspect of this invention, there is provided a plasma processing method in which plasma is generated by the use of a plasma excitation gas and process gas is introduced into the plasma to thereby process an object to be processed, the plasma processing method being characterized in that the process gas includes nitrous oxide gas and the nitrous oxide gas is introduced into the plasma whose electron temperature is less than 2.24 eV.
0019In the plasma processing method, processing using the nitrous oxide gas introduced into the plasma, whose electron temperature is less than 2.24 eV, can be carried out by introducing the plasma excitation gas into a process chamber from an upper shower plate, generating the plasma under the upper shower plate, causing the plasma to pass through a lower shower plate provided under the upper shower plate so as to reach the object to be processed, and introducing the nitrous oxide gas from the lower shower plate into the plasma under the lower shower plate.
0020According to this invention, there is provide a method for manufacturing an electronic device, characterized by comprising a step of carrying out an oxynitriding process to the object to be processed by the use of the plasma processing method.
0021Further, there is obtained a manufacturing method for manufacturing a semiconductor device product, a liquid crystal display device produce, or an organic EL display device product, which is characterized by carrying out a plasma process by the use of the foregoing plasma processing method.
Effect of the Invention
0022As described above, according to this invention, it becomes possible to suppress the production of ions, which damage an oxynitride film, by suppressing dissociation. Further, it also becomes possible to efficiently produce oxynitriding species.
0023This invention is particularly effective for oxynitriding that uses nitrous oxide, so that it becomes possible to form a high-quality oxynitride film. However, this invention is not limited to this nitrous oxide, but enables formation of a high-quality oxynitride film by suppressing dissociation even in another oxynitriding process using ammonia or the like.
0024It is known that, in this invention, leakage current can be reduced by forming a high-quality oxynitride film, which is quite effective in improving the storage properties of a memory or the like.
BRIEF DESCRIPTION OF THE DRAWINGS
0025[<figref idref="DRAWINGS">FIG. 1</figref>] is a sectional view of a plasma processing apparatus in an embodiment of this invention.
0026[<figref idref="DRAWINGS">FIG. 2</figref>] shows the measurement results of radicals in the embodiment of this invention.
0027[<figref idref="DRAWINGS">FIG. 3</figref>] shows a spectrum in the embodiment of this invention.
0028[<figref idref="DRAWINGS">FIG. 4</figref>] shows a spectrum in the embodiment of this invention.
0029[<figref idref="DRAWINGS">FIG. 5</figref>] shows the leakage current measurement results in the embodiment of this invention.
0030[<figref idref="DRAWINGS">FIG. 6</figref>] shows the measurement results of radicals in the embodiment of this invention.
0031[<figref idref="DRAWINGS">FIG. 7</figref>] is a device sectional view in Example 1 of this invention.
0032[<figref idref="DRAWINGS">FIG. 8</figref>] is a device sectional view in Example 1 of this invention.
0033[<figref idref="DRAWINGS">FIG. 9</figref>] is a device sectional view in Example 1 of this invention.
0034[<figref idref="DRAWINGS">FIG. 10</figref>] is a device sectional view in Example 1 of this invention.
0035[<figref idref="DRAWINGS">FIG. 11</figref>] is a device sectional view in Example 1 of this invention.
0036[<figref idref="DRAWINGS">FIG. 12</figref>] is a device sectional view in Example 1 of this invention.
0037[<figref idref="DRAWINGS">FIG. 13</figref>] is a device sectional view in Example 2 of this invention.
0038[<figref idref="DRAWINGS">FIG. 14</figref>] is a device sectional view in Example 2 of this invention.
0039[<figref idref="DRAWINGS">FIG. 15</figref>] is a device sectional view in Example 2 of this invention.
0040[<figref idref="DRAWINGS">FIG. 16</figref>] is a device sectional view in Example 2 of this invention.
0041[<figref idref="DRAWINGS">FIG. 17</figref>] is a device sectional view in Example 2 of this invention.
0042[<figref idref="DRAWINGS">FIG. 18</figref>] is a device sectional view in Example 2 of this invention.
DESCRIPTION OF SYMBOLS
0043<b>101</b>: vacuum container
0044<b>102</b>: dielectric member
0045<b>103</b>: plasma excitation gas inlet
0046<b>104</b>: plasma excitation gas introduction passage
0047<b>105</b>: plasma excitation gas outlet
0048<b>106</b>, <b>107</b>, <b>108</b>: O-ring
0049<b>109</b>: radial line slot antenna
0050<b>110</b>: lattice-shaped shower plate
0051<b>111</b>: process gas inlet
0052<b>112</b>: process gas outlet
0053<b>113</b>: stage
0054<b>114</b>: exhaust port
0055<b>115</b>: substrate
0056<b>116</b>: coaxial waveguide
0057<b>117</b>: process chamber
0058<b>118</b>: process gas passage
0059<b>119</b>: slit
0060<b>120</b>: wave delay plate
0061<b>121</b>: plate
BEST MODE FOR CARRYING OUT THE INVENTION
0062<figref idref="DRAWINGS">FIG. 1</figref> is a side sectional view of a plasma processing apparatus according to an embodiment of this invention. The plasma processing apparatus according to the embodiment comprises a vacuum container <b>101</b>, a dielectric member <b>102</b>, a plasma excitation gas inlet <b>103</b>, a plasma excitation gas introduction passage <b>104</b>, a plasma excitation gas outlet <b>105</b>, O-rings <b>106</b>, <b>107</b>, and <b>108</b>, a radial line slot antenna <b>109</b>, a lattice-shaped shower plate <b>110</b>, a process gas inlet <b>111</b>, process gas outlets <b>112</b>, a stage <b>113</b>, and exhaust ports <b>114</b>. A substrate <b>115</b> to be subjected to plasma processing is placed on the stage <b>113</b>. The stage <b>113</b> has a heating mechanism for raising the substrate temperature.
0063On a surface of the dielectric member <b>102</b> on the side opposite to the vacuum container <b>101</b>, there is provided a radial line slot antenna <b>109</b> adapted to radiate a microwave for plasma excitation. The radial line slot antenna <b>109</b> is configured such that a wave delay plate <b>120</b> made of alumina is sandwiched between a copper plate having a thickness of 0.3 mm and formed with a number of slits <b>119</b> and an aluminum plate <b>121</b> and, further, a coaxial waveguide <b>116</b> for supplying the microwave is disposed at the center. The microwave of 2.45 GHz generated by a microwave power supply (not shown) is supplied to the coaxial waveguide <b>116</b> through an isolator and a matching device (not shown either) and then proceeds from the center toward the periphery in the wave delay plate <b>120</b> so as to be substantially uniformly radiated to the side of the dielectric member <b>102</b> through the slits <b>119</b>. The radiated microwave is introduced into a process chamber <b>117</b> through the dielectric member <b>102</b> and ionizes a plasma excitation gas, thereby generating a high-density plasma.
0064In this embodiment, the vacuum container <b>101</b> is formed of aluminum and the dielectric member <b>102</b> is formed of aluminum nitride. The frequency of the plasma excitation microwave is 2.45 GHz. The substrate <b>115</b> is a silicon substrate having a diameter of 200 mm. The microwave radiated from the radial line slot antenna <b>109</b> disposed in the atmosphere ionizes the gas introduced into the vacuum container <b>101</b> through the plasma excitation gas outlet <b>105</b>, thereby generating a plasma.
0065This apparatus is configured such that the plasma excitation gas and a process gas can be ejected from different introduction ports. The plasma excitation gas is ejected into the vacuum container <b>101</b> through the plasma excitation gas outlet <b>105</b>. On the other hand, the process gas is supplied from the process gas inlet <b>111</b> and passes through the inside of the lattice-shaped shower plate <b>110</b> so as to be ejected to the side of the substrate <b>115</b> through the plurality of process gas outlets <b>112</b>.
0066In the illustrated plasma processing apparatus, the lattice-shaped shower plate <b>110</b> is disposed between the dielectric member <b>102</b> and the process substrate <b>115</b> in the process chamber <b>101</b>. This lattice-shaped shower plate <b>110</b> is formed with many process gas outlets <b>112</b> for supplying the process gas from an external process gas source through a process gas passage <b>118</b> formed in the process chamber. The process gas outlets <b>112</b> of the lattice-shaped shower plate <b>110</b> each eject the supplied process gas into a space between the lattice-shaped shower plate <b>110</b> and the process substrate <b>115</b>. The lattice-shaped shower plate <b>110</b> is formed, between the adjacent process gas outlets <b>112</b>, with opening portions each having a size to efficiently pass by diffusion the plasma formed in the space <b>117</b>.
0067In the structure as described above, when the plasma excitation gas is ejected into the vacuum container <b>101</b> from the plasma excitation gas outlet <b>105</b>, the ejected plasma excitation gas is excited by the high-density plasma formed in the space. However, since the plasma excitation gas from the plasma excitation gas outlet <b>105</b> flows toward the space between the lattice-shaped shower plate <b>110</b> and the process substrate <b>115</b> from the space between the plasma excitation gas outlet <b>105</b> and the lattice-shaped shower plate <b>110</b>, components of the process gas that return to the space between the plasma excitation gas outlet <b>105</b> and the lattice-shaped shower plate <b>110</b> are small in amount, so that decomposition of gas molecules due to excessive dissociation caused by exposure to the high-density plasma is small in amount, thereby enabling high-quality substrate processing.
0068By the use of the plasma processing apparatus of <figref idref="DRAWINGS">FIG. 1</figref>, an experiment was conducted in which a silicon substrate was oxynitrided. Kr gas and O<sub>2 </sub>gas for plasma excitation were introduced into the vacuum container from the plasma excitation gas outlet <b>105</b>, nitrous oxide gas was introduced into the vacuum container <b>101</b> from the lattice-shaped shower plate <b>110</b>, and a plasma was produced with an output of 2.0 kW and at a frequency of 2.45 GHz. The pressure inside the vacuum container <b>101</b> was set to approximately 5 Pa (0.04 Torr) and the flow rates were each set to 100 cc. <figref idref="DRAWINGS">FIG. 2</figref> shows the measurement results of NO radicals and N<sub>2</sub>O radicals in the plasma state in this process. In a conventional structure, the production of NO radicals or N<sub>2</sub>O radicals that contribute to oxynitriding was hardly detected. This is caused by the fact that the nitrous oxide gas was excessively dissociated in the plasma, i.e. due to the excitation of the plasma, to produce N<sub>2 </sub>and O<sub>2</sub>. As shown in <figref idref="DRAWINGS">FIG. 3</figref>, it has also been made clear in the actual plasma optical emission measurement that much of the nitrous oxide gas is dissociated into N<sub>2 </sub>and O<sub>2</sub>.
0069On the other hand, in this invention, by introducing the nitrous oxide from the lattice-shaped shower plate <b>110</b>, it is possible to observe N<sub>2</sub>O radicals and NO radicals that serve as oxynitriding species. This is because, as different from the conventional structure, since the space between the lattice-shaped shower plate <b>110</b> and the process substrate <b>115</b> served as a plasma diffusion region, the electron temperature was very low so that excessive dissociation was suppressed.
0070Herein, it has been ascertained according to the measurement that when a plasma is generated in the vacuum container according to the prior art, the electron temperature between the dielectric member and the process substrate is approximately 3.0 eV. On the other hand, it has also been ascertained that when a plasma is generated by the use of the lattice-shaped shower plate that ejects the process gas, the electron temperature in the space between the lattice-shaped shower plate and the process substrate is approximately 1.0 eV. Since the binding energy between a nitrogen molecule and an oxygen atom is approximately 2.24 eV in nitrous oxide, it is possible to suppress excessive dissociation by introducing the process gas through the process gas outlets of the lattice-shaped shower plate.
0071Following it, the production of N<sub>2 </sub>and O<sub>2 </sub>caused by excessive dissociation of the nitrous oxide gas is suppressed and, hence, NO radicals and N<sub>2</sub>O radicals that contribute to oxynitriding can be efficiently produced. As shown in <figref idref="DRAWINGS">FIG. 4</figref>, it is understood by the use of a Fourier transform infrared spectrophotometer that, with respect to introduction of the nitrous oxide gas at 100 cc, approximately 99% is dissociated in the prior art, while, in this invention, the dissociation ratio is 96%, and therefore, there is a difference of approximately four times with respect to the non-dissociated nitrous oxide gas present in the plasma. This shows the state where the dissociation is suppressed so that NO radicals and N<sub>2</sub>O radicals are easily produced.
0072Next, as shown in <figref idref="DRAWINGS">FIG. 5</figref>, a substrate was subjected to an oxynitriding process by the use of the plasma processing apparatus of <figref idref="DRAWINGS">FIG. 1</figref> and the electrical properties thereof were measured. It has been found that, in this invention, the leakage current density of an oxynitride film is low in an electric field of particularly 6.5 MV/cm<sup>2 </sup>or less. This is because N<sub>2 </sub>ions are produced due to the production of N<sub>2 </sub>in the processing of a substrate according to the prior art and these ions reach the substrate in the processing, thereby causing deterioration of the film quality.
0073However, since the production of N<sub>2 </sub>due to excessive dissociation is suppressed by processing the substrate according to this invention, the production of N<sub>2 </sub>ions can also be suppressed following it, so that it becomes possible to reduce deterioration of the substrate during the processing.
0074On the other hand, by the use of an apparatus having the same structure as described above, the same experiment was conducted for nitrogen monoxide. As shown in <figref idref="DRAWINGS">FIG. 6</figref>, the measurement was carried out for NO radicals and N<sub>2</sub>O radicals in a plasma under the same conditions for nitrous oxide.
0075It has been found that also in the case of nitrogen monoxide, both are reduced as compared with the prior art by introducing the gas from the lattice-shaped shower plate. Since the binding energy between an oxygen molecule and a nitrogen molecule is 6.46 eV in nitrogen monoxide, it is understood that excessive dissociation is not produced in the plasma even in the prior art. However, by changing the introduction port of oxygen gas to the lattice-shaped shower plate, the production of N<sub>2</sub>O radicals can be suppressed and substantially only NO radicals can be selectively produced. This is known to be effective in forming a homogeneous oxynitride film because the NO radical has an equal number of oxygen and nitrogen atoms.
0076The reduction in leakage current value in the low electric field region as described above is very effective in improving the storage properties of a memory or the like.
EXAMPLE 1
0077<figref idref="DRAWINGS">FIGS. 7 to 12</figref> are process sectional views for explaining a manufacturing method of cell transistors in a flash memory device.
0078<figref idref="DRAWINGS">FIG. 7</figref> is a sectional view of a P-type Si substrate element-isolated by STI. A tunnel insulating film having a thickness of, for example, 7 nm is formed by the oxynitride film forming method being this invention. In this event, for example, Kr/O<sub>2 </sub>mixed gases are introduced at 1000 sccm/30 sccm, respectively, into the plasma excitation region (electron temperature: approximately 7 eV) in the chamber and N<sub>2</sub>O, NO, or NH<sub>3 </sub>gas is introduced into the plasma diffusion region (electron temperature: approximately 1.0 eV) by the use of the lattice-shaped shower plate, thereby forming the insulating film while generating a microwave-excited plasma in the state where the pressure inside the chamber is set to 133 Pa (1 torr). The insulating film formed by this invention has a feature in that nitrogen is localized in the insulating film/silicon interface and the surface of the insulating film and this nitrogen is effective in suppressing deterioration of the insulating film caused by tunneling of charge in the insulating film. Thereafter, a polycrystalline silicon film of 90 nm is formed over the entire surface of the substrate by the use of a CVD method. Further, an insulating film is formed on the polycrystalline silicon film by the oxynitride film forming method being this invention. In this event, the insulating film is formed by the use of the oxynitriding method as described above. In this invention, since the insulating film can be formed in a low temperature process at 400° C. or less, the insulating film can be formed without changing the surface state of the polycrystalline silicon film. Thereafter, a second-layer polycrystalline silicon film of 150 nm is formed by the CVD method.
0079Then, an interlayer insulating film is formed over the entire surface of the substrate and contact holes connected to source/drain regions are formed, and thereafter, these contact holes are filled with, for example, tungsten (<figref idref="DRAWINGS">FIG. 12</figref>). Then, after forming a wiring layer connected to these tungsten plugs, a surface protective film is formed over the entire surface of the substrate.
EXAMPLE 2
0080<figref idref="DRAWINGS">FIGS. 13 to 18</figref> are process sectional views for explaining a manufacturing method of cell transistors in a flash memory device.
0081<figref idref="DRAWINGS">FIG. 13</figref> is a sectional view of a P-type Si substrate element-isolated by STI. A tunnel insulating film having a thickness of, for example, 7 nm is formed in two stages. In this two-stage forming method, an oxide film of 6.5 nm is first formed by a thermal oxidation method at, for example, 900° C. or by a microwave-excited plasma of, for example, Kr/O<sub>2 </sub>mixed gases and, thereafter, an oxynitride film of 0.5 nm is formed by the oxynitride film forming method of this invention.
0082The formation of the oxynitride film being this invention is carried out such that, for example, Kr/O<sub>2 </sub>mixed gases are introduced at 1000 sccm/30 sccm, respectively, into the plasma excitation region (electron temperature: approximately 3 eV) in the chamber and N<sub>2</sub>O, NO, or NO gas is introduced into the plasma diffusion region (electron temperature: approximately 1.0 eV) by the use of the lattice-shaped shower plate, thereby forming the insulating film while generating a microwave-excited plasma in the state where the pressure inside the chamber is set to 133 Pa (1 torr).
0083The insulating film formed in the two stages as described above has a feature in that the nitrogen concentration in the insulating film/silicon interface and the surface of the insulating film can be optionally controlled according to the formation conditions of the oxynitride film. By carrying out the oxynitriding being this invention after the formation of the thermal oxide film or the plasma oxide film being the conventional technique, it becomes possible to incorporate nitrogen into the interface at low temperature and without damaging the insulating film.
0084This nitrogen in the insulating film interface is effective in suppressing deterioration of the insulating film caused by tunneling of charge in the insulating film. Thereafter, a polycrystalline silicon film of 90 nm is formed over the entire surface of the substrate by the use of the CVD method. Further, an insulating film is formed on the polycrystalline silicon film by the foregoing oxynitride film forming method being this invention. In this invention, since the insulating film can be formed in a low temperature process at 400° C. or less, the insulating film can be formed without changing the surface state of the polycrystalline silicon film.
0085Then, an interlayer insulating film is formed over the entire surface of the substrate and contact holes connected to source/drain regions are formed, and thereafter, these contact holes are filled with, for example, tungsten (<figref idref="DRAWINGS">FIG. 18</figref>). Then, after forming a wiring layer connected to these tungsten plugs, a surface protective film is formed over the entire surface of the substrate.
0086As described above, in the embodiment of this application, by the use of the plasma processing method of this invention, there is obtained the electronic device manufacturing method that can uniformly and efficiently form the oxynitride film.
Contents8
13 sheets
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| Document | Relation | Office | Cited during |
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| JP2000294550A | Cites | Japan | Applicant |
| JP2001500327A | Cites | Japan | Applicant |
| JP2003068731A | Cites | Japan | Applicant |
| JP2003183839A | Cites | Japan | Applicant |
| US2004245584A1 | Cites | United States of America | Search report |
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| Information on status: patent discontinuationPATENT EXPIRED DUE TO NONPAYMENT OF MAINTENANCE FEES UNDER 37 CFR 1.362STCH | STCH | |
| Information on status: patent discontinuationPATENT EXPIRED DUE TO NONPAYMENT OF MAINTENANCE FEES UNDER 37 CFR 1.362STCH | STCH | |
| Lapse for failure to pay maintenance feesLapsedLAPS | LAPS | |
| Maintenance fee reminder mailedREMI | REMI | |
| AssignmentAS | AS | |
| AssignmentAS | AS |
Numbers
- Publication
- 7928018
- Application
- 10594895
Titles
- English
- Plasma processing method and method for manufacturing an electronic device
Patent term adjustment
- A delay
- +473 daysthe office missed an examination deadline
- B delay
- +251 dayspendency past three years
- Applicant delay
- −179 days
- Net adjustment
- 545 days
Classification
- CPC, 11
- H10P95/00
- H01J2237/3387
- H10B69/00
- H10B41/30
- H10B43/30
- H10D64/035
- H10D64/037
- H10P14/69433
- H10P14/662
- H10P14/6319
- H10P14/6336
- IPC, 13
- H01L21 31
- H01L21 469
- H01L21 02
- C23C16 00
- H05H1 46
- H01L21 3105
- H01L21 314
- H01L21 318
- H01L21 8247
- H10B20 00
- H10B69 00
- H10D30 68
- H10D30 69
- USPC, 10
- 438769000
- 11872300R
- 1187230MW
- 257411000
- 438765000
- 438771000
- 438772000
- 438775000
- 438776000
- 438777000